JPH1090047A - Weighing meter - Google Patents

Weighing meter

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Publication number
JPH1090047A
JPH1090047A JP26511196A JP26511196A JPH1090047A JP H1090047 A JPH1090047 A JP H1090047A JP 26511196 A JP26511196 A JP 26511196A JP 26511196 A JP26511196 A JP 26511196A JP H1090047 A JPH1090047 A JP H1090047A
Authority
JP
Japan
Prior art keywords
value
creep
load
time
temperature
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP26511196A
Other languages
Japanese (ja)
Inventor
Koji Oguma
耕二 小熊
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Tanita Corp
Original Assignee
Tanita Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Tanita Corp filed Critical Tanita Corp
Priority to JP26511196A priority Critical patent/JPH1090047A/en
Publication of JPH1090047A publication Critical patent/JPH1090047A/en
Pending legal-status Critical Current

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Abstract

PROBLEM TO BE SOLVED: To remove error with ease by calculating change amount of enumerated value due to creep as a function of a read enumerated value and that from loaded point till measurement time point, and taking as a load value after removing the change amount from the read enumerated value. SOLUTION: A correction amount Δ of creep error value occurring at each measurement time is represented in Δ=-(A×N<2> +B×N+C)/(D×T<2> +T+E). Where, Δ is creep correction amount, N is an enumerated value obtained with a load, T is a time period under load, and A-E are a constant which is specific to a weighing meter. A display value NW at a time TN is obtained form equation NW=NTN-(ΔNT1 +ΔNT2 ...+ΔNTN)(ΔNTn is creep error value at time TN). With a temperature censor and an A/D converter, a temperature at measurement is obtained, and t-t0 =Δt, where (t) is temperature at measurement and t0 is temperature constant. While, A=aΔt, B=bΔt, C=cΔt, D=dΔt, E=eΔt, constants A-E are calculated. a-e, tδ0Χ are obtained according to the material.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】 電子式重量計に関し、その
測定精度を維持する方法に関する。
[0001] 1. Field of the Invention [0002] The present invention relates to an electronic weighing scale and a method for maintaining the measurement accuracy.

【0002】[0002]

【従来の技術】 荷重とバランスする起歪体の材質や形
状、起歪体に貼着され、起歪体のひずみ量を電気量に変
換するひずみゲージのベースとなる絶縁材の材質や厚み
及び、ひずみ抵抗のパターン形状等、それぞれクリープ
による作用と効果が異なる要素を、打ち消し合って、ト
ータルとして見掛け上クリープがゼロとなる様に、秤の
仕様毎に、選択し調整して設計していた。
2. Description of the Related Art The material and shape of a strain-generating body that balances a load, the material and thickness of an insulating material attached to the strain-generating body and serving as a base of a strain gauge that converts the amount of strain of the strain-generating body into an electric quantity, and Each element of the scale was selected and adjusted so that the elements with different effects and effects due to creep, such as the pattern shape of the strain resistance, cancel each other out, and the apparent creep becomes zero as a whole. .

【0003】 クリープによる作用と効果の異なる要素
の総合で、クリープ誤差をゼロにするには、使用する素
材の制限も厳しく、組み合わせには多大な時間と費用を
要する物であり、然も、秤の仕様が異なる毎に秤の仕様
に合わせて設計することは多くの時間と費用を要した。
[0003] In order to eliminate the creep error by combining the elements having different effects and effects due to creep, the materials to be used are severely restricted, and the combination requires a great deal of time and money. It took a lot of time and money to design according to the specifications of the scale each time the specifications of the weighing differed.

【0004】[0004]

【発明が解決しようとする課題】 本発明の課題は、よ
り簡単に、低コストでクリープ誤差のない秤を得ること
である。
SUMMARY OF THE INVENTION It is an object of the present invention to provide a scale which is simpler, less expensive and free of creep errors.

【0005】[0005]

【課題を解決するための手段】 クリープによるカウン
ト値の変化分を、読み取りカウント値と荷重が負荷され
てから計測時点までの時間の関数として算出し、読み取
りカウント値からクリープによるカウント値の変化分を
取り除いた値を荷重の重量とする。
Means for Solving the Problems The change in the count value due to creep is calculated as a function of the read count value and the time from when the load is applied to the time of measurement, and the change in the count value due to creep is calculated from the read count value. The value from which is removed is defined as the weight of the load.

【0006】[0006]

【作用】 荷重を負荷したとき得られるカウント値は、
時間が経過するに従って変化することが知られている。
これは起歪体の荷重による変形が実際は「擬弾性」によ
るものであり、塑性変形に近い状態になり、時間が経過
するに従って、変形が進む為であり、特に起歪体とひず
み抵抗との絶縁体となる樹脂材であるひずみゲージのベ
ースはこの傾向が顕著に現れる。
[Action] The count value obtained when a load is applied is
It is known that it changes over time.
This is because the deformation due to the load of the flexure element is actually due to "pseudoelasticity", and it becomes a state close to plastic deformation, and the deformation progresses as time passes. This tendency is conspicuous in the strain gauge base, which is a resin material serving as an insulator.

【0007】 ある荷重Wを負荷した時のカウント値の
変化を図2に示す。負荷した瞬間T0 のカウント値NT0
を真値とすると、時間が経過するに従って誤差が大きく
なり、その増加の割合は、時間が経過するに従って小さ
くなる。この増加の割合は、T0 を基準とした時間の逆
数におおよそ比例するが、厳密には差異がみられ、逆数
の自乗の項が必要になる。つまり、T1で生じた誤差を
ΔNT1とすると、比例定数をKとおいてΔNT1=NT1
T0=K/(DT1 2+T1+E)で表される。DとEは
各計量器固有の定数である。以下同様に ΔNT2=NT2−NT1=K/(DT2 2+T2+E) ΔNT3=NT3−NT2=K/(DT3 2+T3+E) ΔNT4=NT4−NT3=K/(DT4 2+T4+E)と計算
できる。
FIG. 2 shows a change in the count value when a certain load W is applied. Count value N T0 of moment T 0 when load is applied
Is a true value, the error increases as time elapses, and the rate of increase decreases as time elapses. Although the rate of this increase is roughly proportional to the reciprocal of the time with reference to T 0 , there is a strict difference, and a term of the square of the reciprocal is required. That is, when the error produced by T 1 and .DELTA.N T1, the proportionality constant at the K ΔN T1 = N T1 -
Represented by N T0 = K / (DT 1 2 + T 1 + E). D and E are constants specific to each measuring instrument. The following Similarly ΔN T2 = N T2 -N T1 = K / (DT 2 2 + T 2 + E) ΔN T3 = N T3 -N T2 = K / (DT 3 2 + T 3 + E) ΔN T4 = N T4 -N T3 = It can be calculated as K / (DT 4 2 + T 4 + E).

【0008】 T1 での真の値は、上記クリープ誤差Δ
T1を引いた値であるから、クリープ補正量は−ΔNT1
で表せる。つまり、表示値NWは、 NW=NT1−ΔNT1=NT1−(NT1−NT0)=NT0 となり、真値となることが解る。T4での表示値NWに対
する補正量は、その間のクリープ補正量を合算したもの
になる。 NW=NT4−(ΔNT1+ΔNT2+ΔNT3+ΔNT4)=N
T0 つまり、Tnでのクリープ誤差値は、 ΔNTn=NTn−NTn-1=K/(DTn2+Tn+E) で表され、Tnでの表示値は NW=NTn−(ΔNT1+ΔNT2+……+ΔNTn-1+ΔN
Tn) で計算される。
The true value at T 1 is the creep error Δ
Since a value obtained by subtracting the N T1, creep correction amount -DerutaN T1
Can be represented by That is, the display value N W is N W = N T1 −ΔN T1 = N T1 − (N T1 −N T0 ) = N T0 , and it is understood that the display value N W is a true value. Correction amount for the display value N W at T 4 will that the sum therebetween creep correction amount. N W = N T4 − (ΔN T1 + ΔN T2 + ΔN T3 + ΔN T4 ) = N
T0 That is, creep error value at T n is expressed by ΔN Tn = N Tn -N Tn- 1 = K / (DT n2 + T n + E), the display value at T n is N W = N Tn - ( ΔN T1 + ΔN T2 +... + ΔN Tn-1 + ΔN
Tn ).

【0009】 比例定数Kは、荷重によって異なり、負
荷後一定時間における各荷重とクリープ誤差量とは図3
に示す関係にある。クリープ誤差は、荷重が大きいほ
ど、荷重に対し比例より大きな割合で増え、K=AW2
+BW+Cで近似される。(W:荷重、 A,B,C:
定数) 荷重は荷重によって得られるカウント値Nを使って求め
られ、比例定数KはK=AN2+BN+Cとして求めら
れる。つまり、クリープ補正量は、 Δ=−(A×N2+B×N+C)/(DT2+T+E) で求めることができる。
The proportional constant K varies depending on the load. Each load and the amount of creep error during a certain time after the load are shown in FIG.
The relationship is shown in The creep error increases as the load increases, at a rate larger than the proportional to the load, and K = AW 2
+ BW + C. (W: Load, A, B, C:
Constant) The load is determined using a count value N obtained by the load, and the proportional constant K is determined as K = AN 2 + BN + C. That is, the creep correction amount can be obtained by Δ = − (A × N 2 + B × N + C) / (DT 2 + T + E).

【0010】[0010]

【実施の形態】 図1に本発の明実施例のブロック図を
示す。各計測時間に生じるクリープ誤差値を求めるクリ
ープ補正式をΔ=−(A×N2+B×N+C)/(DT2+
T+E)としてクリープ補正量を求め、(Δ:クリープ
補正量、N:荷重により得られたカウント値、T:荷重
がかけられた時間、A、B、C、D、E:重量計固有の
定数) Tnでの表示値、NWを NW=NTn−(ΔNT1+ΔNT2+……+ΔNTn-1+ΔN
Tn) で計算により求める。温度センサとA/D変換器を用い
て、計測時の温度を得て、計測時の温度をt、温度定数
をt0とおき、A=a(t−t0)、B=b(t−
0)、C=c(t−t0)、D=d(t−t0)、E=
e(t−t0)として上記定数、A,B,C,D及びE
を計算により求める。 a,b,c,d,eおよびt0
は、実際の材料に応じて求められる値である。 また、
各温度でのA、B、C、D、Eをあらかじめ記憶してお
き、測定された温度によって、それに対するA,B,
C,D,Eを呼出し、使用する事は有効である。
FIG. 1 is a block diagram showing a bright embodiment according to the present invention. The creep correction formula for obtaining the creep error value generated at each measurement time is represented by Δ = − (A × N 2 + B × N + C) / (DT 2 +
The creep correction amount is calculated as (T + E), (Δ: creep correction amount, N: count value obtained by load, T: time when load is applied, A, B, C, D, E: constants specific to weighing scale ) display value at T n, N W and N W = N Tn - (ΔN T1 + ΔN T2 + ...... + ΔN Tn-1 + ΔN
Tn ) is obtained by calculation. Using a temperature sensor and A / D converter, with the temperature at the time of measurement, the temperature at the time of measurement t, the temperature constant t 0 Distant, A = a (t-t 0), B = b (t −
t 0 ), C = c (t−t 0 ), D = d (t−t 0 ), E =
e (t−t 0 ), the above constants, A, B, C, D and E
Is obtained by calculation. a, b, c, d, e and t 0
Is a value determined according to the actual material. Also,
A, B, C, D, and E at each temperature are stored in advance, and A, B, and
It is effective to call and use C, D and E.

【0011】[0011]

【発明の効果】 以上述べた如く、荷重センサのクリー
プ誤差量を荷重値と荷重された時間の関数として求め読
み取り値を補正することで荷重の真値を得ることが出
来、使用素材の特性の制限も少なく秤の用途、使用に合
わせた設計が出来、クリープ値が補正された正確な測定
が出来る秤が、低コストで作製できる。
As described above, the true value of the load can be obtained by obtaining the creep error of the load sensor as a function of the load value and the load time, and correcting the read value. The scale can be designed according to the use and use of the scale with few restrictions, and a scale capable of accurate measurement with corrected creep value can be manufactured at low cost.

【図面の簡単な説明】[Brief description of the drawings]

【図1】 本発明の実施例のブロック回路図FIG. 1 is a block circuit diagram of an embodiment of the present invention.

【図2】 荷重を負荷したときのカウント値と時間の関
係を示す図
FIG. 2 is a diagram showing a relationship between a count value and time when a load is applied.

【図3】 負荷後一定時間後の荷重とクリープとの関係
を示す図
FIG. 3 is a diagram showing a relationship between a load and a creep after a certain time after the load.

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 荷重をカウント値に変換して計量する重
量計に於いて、荷重が負荷された時間を計測し、得られ
たカウント値と計測に要した時間の項を含むクリープ補
正式を有し、補正式から得られた値を各々の時間に生じ
たクリープ誤差補正値として、前記カウント値とクリー
プ誤差補正値とを逐次合算した値を表示値とするするこ
とを特徴とする重量計。
In a weighing scale that converts a load into a count value and weighs it, a time during which the load is applied is measured, and a creep correction formula including a term of the obtained count value and a time required for the measurement is calculated. Wherein the value obtained from the correction formula is used as a creep error correction value generated at each time, and a value obtained by successively adding the count value and the creep error correction value is used as a display value. .
【請求項2】 各の時間に生じるクリープ誤差値を求め
るクリープ補正式をΔ=−(A×N2+B×N+C)/
(DT2+T+E)とすることを特徴とする請求項1に記
載の重量計。上記補正式において、Δはクリープ補正量
を、Nは荷重により得られたカウント値を、Tは荷重が
かけられた時間であり、A、B、C、D、Eはそれぞれ
重量計固有の定数である。
2. A creep correction equation for calculating a creep error value generated at each time is represented by Δ = − (A × N 2 + B × N + C) /
2. The weighing scale according to claim 1, wherein (DT 2 + T + E). In the above correction formula, Δ is the amount of creep correction, N is the count value obtained by the load, T is the time during which the load is applied, and A, B, C, D, and E are constants specific to the weighing scale, respectively. It is.
【請求項3】 荷重センサの温度を得る手段を有し、ク
リープ補正式の定数、A、B、C、DおよびEを、測定
時の温度の関数とすることを特徴とする請求項2に記載
の重量計。
3. The method according to claim 2, further comprising means for obtaining the temperature of the load sensor, wherein the constants A, B, C, D and E of the creep correction equation are functions of the temperature at the time of measurement. Weight scale as described.
JP26511196A 1996-09-17 1996-09-17 Weighing meter Pending JPH1090047A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP26511196A JPH1090047A (en) 1996-09-17 1996-09-17 Weighing meter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP26511196A JPH1090047A (en) 1996-09-17 1996-09-17 Weighing meter

Publications (1)

Publication Number Publication Date
JPH1090047A true JPH1090047A (en) 1998-04-10

Family

ID=17412771

Family Applications (1)

Application Number Title Priority Date Filing Date
JP26511196A Pending JPH1090047A (en) 1996-09-17 1996-09-17 Weighing meter

Country Status (1)

Country Link
JP (1) JPH1090047A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007003523A (en) * 2005-06-21 2007-01-11 Mettler-Toledo Ag Method for optimizing behavior of force measuring device, and force measuring device
JP2009068994A (en) * 2007-09-13 2009-04-02 Yamato Scale Co Ltd Creep error compensation device and method, and creep recovery error compensation device and method for load detector
JP2011033374A (en) * 2009-07-30 2011-02-17 Yamato Scale Co Ltd Device and method for compensating creep error

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007003523A (en) * 2005-06-21 2007-01-11 Mettler-Toledo Ag Method for optimizing behavior of force measuring device, and force measuring device
JP2009068994A (en) * 2007-09-13 2009-04-02 Yamato Scale Co Ltd Creep error compensation device and method, and creep recovery error compensation device and method for load detector
JP2011033374A (en) * 2009-07-30 2011-02-17 Yamato Scale Co Ltd Device and method for compensating creep error

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